Simulation and experimental validation of heat transfer in a novel hybrid solar panel
, Z.F. Yuan, P.H. Lee, H.M. Yin
Department of Civil Engineering and Engineering Mechanics, Columbia University, 610 SW Mudd, 500 West 120th Street, New York, NY 10027, United States
a r t i c l e
i n f o
Article history: Received 18 March 2011
Received in revised form 30 September 2011 Available online 21 October 2011 Keywords:
Finite element method Functionally graded material Heat transfer
Hybrid solar panel Solar energy
a b s t r a c t
A hybrid solar panel has been invented to integrate photovoltaic (PV) cells onto a substrate through a functionally graded material (FGM) with water tubes cast inside, through which water serves as both heat sink and solar heat collector. Therefore, the PV cells can work at a relatively low temperature while the heat conduction to the substrate can be minimized. Solar panel prototypes have been fabricated and tested at different water ﬂow rates and solar irradiation intensities. The temperature distribution in the solar panel is measured and simulated to evaluate the performance of the solar panel. The ﬁnite element simulation results are very consistent with the experimental data. The understanding of heat transfer in the hybrid solar panel prototypes will provide a foundation for future solar panel design and optimiza-tion. The ﬁnite element model is general and can be extended for different material design and other size of panels.
Ó 2011 Elsevier Ltd. All rights reserved.
Solar panels have become a very promising and popular ap-proach to collect solar energy. Currently solar panel products in market mainly use photovoltaic (PV) cells for the electricity gener-ation. PV technology has achieved tremendous progress since the invention in 1839. However, there is still signiﬁcant research need in the aspects of efﬁciency improvement and life-cycle cost reduc-tion. For the single crystalline single junction Si technology, the conversion efﬁciency keeps lower than 30%[1,2]. Thus a large por-tion of solar energy is wasted through heat dissipapor-tion [3,4]. Although some emerging technologies can considerably improve energy utilization efﬁciency, such as multi-junction cells, opti-cal frequency shifting, multiple exciton generation cells, hot carrier cellsand concentration photovoltaic system, these technologies require high cost and complex service conditions, and thus have not been commercially used in solar rooﬁng panel yet.
Solar thermal technology provides another way to use the ther-mal energy of solar insolation. Solar therther-mal collectors have been applied to domestic (bath, cooking, space heating and swimming pool heating etc.) and commercial sectors (pre-heating of boiler and hospitals etc.). Typically, energy payback time (EPBT) for solar thermal system is much less than that of PV systems. The EPBT of PV system can be reduced by using it in a hybrid system integrat-ing PV with solar thermal components, such as hot water (HW) tubes. The combination of the above two approaches is not a
simple superposition of the materials and costs, but provides a via-ble solution to signiﬁcantly increase overall energy utilization efﬁ-ciency while alleviating the disadvantages of a single approach
. A PV-thermal collector enables heat harvesting while improv-ing the PV utilization efﬁciency by controllimprov-ing the temperature of PV modules. Currently, some groups have studied the performance of PV-thermal hybrid systems[12,13], which provide the good jus-tiﬁcations of the solar hybrid approaches.
In this work, we developed a novel functionally graded material (FGM) based hybrid solar panel asFig. 1 . A PV surface layer, transferring the photo energy into electricity, is bonded to a struc-tural substrate plate through a functionally graded material (FGM) interlayer. The FGM contains aluminum powder dispersed in a high density polyethylene (HDPE) matrix with a graded micro-structure seen in the left top ofFig. 1. Water pipelines are cast within the FGM to control the panel’s temperature. The substrate, namely, plastic lumber made of recycled polymer, provides mechanical loading support and heat insulation of the roof.
FGMs are characterized by continuous variation of the volume fraction of the constituents. FGMs have attracted signiﬁcant interests among researchers and engineers because of their unique thermo-mechanical properties and microstructures[16–18]. The effective material properties, such as thermal conductivity, vary continuously in the gradation direction and keep constant in the plane normal to the gradation direction . In the following experiment, the Al powder concentration gradually decreases from the top to the bottom. Thus the thermal conductivity also decreases gradually from the top to the bottom of the FGM layer.
The remainder of this paper is organized as follows: Section2
introduces the hybrid solar panel prototype fabrication, and testing instruments and procedure. In Section 3, the irradiation space 0017-9310/$ - see front matter Ó 2011 Elsevier Ltd. All rights reserved.
⇑Corresponding author. Tel.: +1 347 371 2259; fax: +1 212 854 6267. E-mail address:firstname.lastname@example.org(D.J. Yang).
Contents lists available atSciVerse ScienceDirect
International Journal of Heat and Mass Transferj o u r n a l h o m e p a g e : w w w . e l s e v i e r . c o m / l o c a t e / i j h m t
uniformity of the metal halide lamp and the temperature distribu-tion of the solar panel are characterized. A ﬁnite element model (FEM) is implemented using ABAQUS to simulate the thermal transfer characteristics of the solar panel. The FEM results are com-pared with the experimental data. The overall energy efﬁciency of the solar panel is evaluated based on the testing results. Finally, some conclusions are drawn in Section4.
2. Experimental set up and procedure 2.1. Solar panel fabrication
The hybrid solar panel has been fabricated for photovoltaic (PV), hot water utilization through a multilayered conﬁguration. The PV cells used in the panels are commercial single crystalline Si solar cells with an open circuit voltage Vocof 0.55 V, short circuit current Iscof 4400 mA and an energy conversion efﬁciencypvof 13% at room temperature (25 °C). The length, width and thickness of the solar cell are 12.5 cm, 12.5 cm and 270 m, respectively. Pure Al powder and high density polyethylene (HDPE) matrix are used to fabricate the FGM layer. The thermal conductivity of Al and HDPE are 238 and 0.26 W/m K, respectively. The HDPE and Al powder are mixed layer by layer with a continuously changing proportion such as 50% Al volume fraction in the bottom and pure HDPE in the top of a mold. The mix within the mold is baked in a vacuum at 200 °C for 1.5 h and is then solidiﬁed with dimensions of 30.5 30.5 1.5 cm. A vacuum sintering process is employed to bond the FGM layer with the plastic lumber substrate which is made of recycled polymeric materials. The water tubes made with cop-per (Cu) pipes with a diameter of 6 mm are cast into the FGM layer with a separation of 2.5 cm. Thermal conductive paste with a conductivity of 1.9 W/m K is used as an adhesive between the
PV, and FGM layers. The complete panels are degassed in a vacuum oven at 90 °C for 2 h.
The photovoltaic (PV) layer can transfer a portion of the solar energy to electricity. The thin PV layer improves the heat conduc-tion and structural integrity within the panel, and protects the polymer materials underneath from UV radiation. The high per-centage of aluminum (Al) powder in top surface of the FGM makes rapidly heat transfer into the water tubes, but below them the heat conduction is blocked by the HDPE and the plastic lumber sub-strate. The hot water, whose temperature is partially controlled by the ﬂow rate, can be directly utilized by water heating systems for domestic usage.
2.2. Testing method
Eight T type thermal couples (±1 °C) are attached on the panels to detect the temperature distribution of the PV cells and water. The solar panels are tested in a solar room equipped with a metal halide lamp, which can provide irradiation up to 4 KW/m2. The pa-nel is ﬁxed on a wood frame with 45° tilt angle so that the papa-nel surface is normal to the irradiation. A pyranometer is used to mea-sure and calibrate the solar irradiation. A mass ﬂow meter is used to control the cooling water ﬂow rate. The experimental data is col-lected with the data acquisition system. The whole system testing set up is shown inFig. 2.
The performance of the solar panels are characterized in the following way: The solar panels are put in the solar room under different irradiations of 850 and 1100 W/m2. Before the water ﬂow starts, the solar panel surface temperature is automatically mea-sured with an interval of 2 s until the panel reaches a stabilized Nomenclature
C speciﬁc heat
D copper tube diameter Ein input solar energy Erad radiation heat loss Econ convection heat loss Epv PV cell energy
Ewater thermal energy from water hc convection coefﬁcient of air hw convection coefﬁcient of water Isc short circuit current
k effective thermal conductivity
K thermal conductivity m mass of water Nu Nusselt number s Stefan–Boltzmann Constant Tpv PV cell temperature Tam ambient temperature Vac open circuit voltage
gpv PV cell efﬁciency / volume fraction
DT temperature difference
esurface emissivity of silicon
temperature. Then the water ﬂow is introduced with the inlet water temperature at 20 °C. The ﬂow rate is controlled by the mass ﬂow meter at 33 and 66 ml/min for the irradiations of 850 and 1100 W/m2, respectively. These water ﬂow rates are determined by some trial-error tests so that the panel can be effectively cooled and the outlet water temperature keeps in a range between 32–34 °C. The irradiation levels are chosen to cover a small range around the AM1.5 (1000 W/m2) condition. The PV cell and water temperatures are recorded continuously until the panel tempera-ture stabilizes again.
3. Results and discussion
3.1. Irradiation space uniformity
During the tests, we use a metal halide lamp to simulate solar irradiation. The space uniformity of the irradiation is examined through 25 point measurement on the panel surface where is equally divided into 25 square areas. The 25 measuring points are uniformly distributed in the 25 square areas. Two different irradiation settings of 850 and 1100 W/m2 are tested. The two dimensional irradiation contour maps are shown inFig. 3. Irradia-tion maps are approximately symmetric within the panel with re-spect to the center point which receives the highest irradiations. It is reasonable as the panel surface is normal to the irradiation with the center aligned to the lamp. The coefﬁcients of variation of the 25 point measurements are 2.9% and 3.3% for the irradiation of 850 and 1100 W/m2, respectively.
3.2. Temperature distribution
Seven thermal couples are attached on the surface of the solar panel to evaluate the temperature distribution, as shown in
Fig. 4, which also indicates the direction of water ﬂow along the water tube by the arrows. For the data analysis conveniences, the sensor point number sequence follows the water ﬂow direction. The eighth thermal couple is attached in the outlet water tube to test the outlet water temperature.
Fig. 5(a) shows the equilibrium temperature of the 8 points without and with water ﬂow of 33 ml/min under the irradiation of 850 W/m2, and Fig. 5(b) without and with water ﬂow of 66 ml/min under the irradiation of 1100 W/m2. It can be seen that even the irradiation map has the center high pattern, most region of solar panel still can be uniformly heated up, as the variation of the high equilibrium temperatures among the 7 points is within
±2 °C. With the water ﬂow introduced, the temperatures of the 7 points monotonically increase with the point number sequence. As the higher the point number, the more thermal energy the water absorbed, and the less the cool effect.Fig. 6shows the tem-perature variation with time at two different irradiations and water ﬂow conditions. Before the water ﬂow starts, the solar panel surface temperatures increase fast with time and then gradually saturate at around 50 and 55 °C at the time around 7700–8100 s for the irradiation of 850 and 1100 W/m2, respectively. With the water ﬂow introduced, the temperatures sharply dropped and then stabilized at around 32–38 °C. The outlet water temperature is around 32–34 °C. These results show that water tubes integrated with FGM layers can effectively cool the PV cells.
3.3. Finite element simulation
3.3.1. FEM and multilayer discretization
A commercial software package ABAQUS is used to simulate heat transfer across the solar panel. The model and grid generation of solar panel is shown inFig. 7. The panel is discretized into eight layers in vertical direction including PV cells, thermal conductive
Fig. 3. Contour map of the solar irradiation on the panel surface for (a) 850 W/m2
and (b) 1100W/m2
paste, and six FGM layers with gradient variation of percentage of HDPE and aluminum. Within layer 4 and 5, there are 11 water tubes uniformly distributed. The thickness of copper tube is 1 mm and inner diameter is 4 mm. More grids are generated around tube area for better accuracy due to the curvature of water tube and ﬂuid heat transfer characteristics.
3.3.2. Material speciﬁcation
Within each FGM layer, material is assumed to be homoge-neous, and the effective thermal conductivity can be calculated based on following equation.
k ¼ kB /
a1 þ/b2 4 h i þ ð1 /Þ /kB kA
a1 þ /b2 4 h i þ ð1 /Þ ð1Þ
where kA, ksis the thermal conductivity of particle phase A and ma-trix B, respectively, which stand for two constitution particulate materials for the FGM layer, e. g. the Al and HDPE powders. / is vol-ume fraction of particle phase A, and
a, b are deﬁned as
a¼ 3kA kAþ 2kB
;b¼ kA kB
kAþ 2kB ð2Þ
By using the thermal conductivity values of 238 and 0.26 W/m K for Al and HDPE, respectively, the effective thermal conductivity of HDPE/Al matrix with different volume fraction can be calculated.
Table 1lists the dimension and properties of each layer and mate-rial that are used in the ﬁnite element simulation.
3.3.3. Thermal energy circulation
The total input solar energy Einis simulated using the numerical integration of the 25 point irradiation value shown inFig. 3. A one dimensional thermal conduction model is used to simulate the heat transfer between and within each layer. The radiation and convection heat loss can be calculated as:
Erod¼s ðT4pm T
Econ¼ hc ðTpm TamÞ ð4Þ
e, s, hc, Tpvand Tamare the average surface emissivity of sil-icon 0.6, Stefan–Boltzmann Constant 5.67 108W/m2K4, con-vection coefﬁcient of air 5 W/m2K, panel surface temperature and ambient temperature, respectively[20,21]. The solar room ambient temperature, Tam, is also continuously recorded with the range from 25 to 35 °C. A forced convention model is used to describe the heat transfer between the water and the FGM layers. The Nusselt num-ber is deﬁned as
where hwis convection heat transfer coefﬁcient of water, D is water tube diameter, and k is thermal conductivity of water, which is approximately 0.58 W/m K. Normally, for fully developed pipe ﬂow with uniform wall heat ﬂux, Nusselt number is given by Fig. 5. Equilibrium temperatures of each point at conditions of (a) irritation:
, water ﬂow rate: 33 ml/min, (b) irritation: 1100 W/m2
, water ﬂow rate: 66 ml/min.
Fig. 6. Temperature variation with time diagram for (a) irritation: 850 W/m2
, water ﬂow rate: 33 ml/min, (b) irritation: 1100 W/m2
Nu = 48/11 = 4.36. For this model, D is the copper pipe diameter of 4 mm, so the heat convection transfer coefﬁcient of water is
D ¼ 632:2
m2 K ð6Þ
For simplicity, we assume the water temperature increases linearly along the water ﬂow path, which can be effectively justiﬁed by the data inFig. 5. Once we know the temperatures of inlet water and outlet water at one time, the temperature distribution of water ﬂow along the full path within the FGM layer can be approximated for heat transfer simulation in the FEM.
3.3.4. Simulation results
Fig. 8shows the equilibrium temperature space distribution in the panel at the condition of the irradiation at 1100 W/m2and the water ﬂow rate at 66 ml/min. The red1color and blue color stand for high and low temperatures, respectively. Before the water ﬂow starts, the whole panel surface is uniformly heated up, as depicted inFig. 8(a). When the water ﬂow was introduced, the overall panel surface temperature decreased and linearly distributed from the inlet to outlet position, as shown inFig. 8(b), which is consistent with the experimental observations inFig. 5, where the tempera-tures of point 1–7 monotonically increase with the point number. The temperature variation with time of the 7 points on the pa-nel are also simulated and compared to the experimental results.
Fig. 7. FEM and grid generation for (a) whole of solar Panel, (b) close up of the cross section, and (c) close up of a water tube.
Thickness and properties of each material used in FEM simulation. Layer/material Thickness (mm) Density g/cm3 Speciﬁc heat J/g K Thermal conductivity W/m K 1, PV cell (Si) 0.27 2.33 0.7 130
2, Silicone thermal paste 0.30 2.6 0.7 1.9
3, 50% HDPE 2 1.83 1.58 1.13 4, 60% HDPE 2 1.65 1.74 0.83 5, 70% HDPE 2 1.48 1.85 0.62 6, 80% HDPE 2 1.30 1.98 0.46 7, 90% HDPE 2 1.13 2.12 0.35 8, 100% HDPE 13 0.95 2.25 0.26 Copper tube 1 8.94 0.39 401 Water – 1 4.18 0.58
Fig. 8. Temperature space distributions of the panel at (a) 1100 W/m2
irradiation without water ﬂow, (b) 1100 W/m2
irradiation with water ﬂow of 66 ml/min.
For interpretation of color in Fig. 8, the reader is referred to the web version of this article.
As the data proﬁles of both experiment and simulation for the 7 points are practically the same, only the results of point 4 are shown inFig. 9. Basically, the FEM simulation results well ﬁt to the experiments. There is a gap (8% mismatch) between the FEM simulations and experiment data at the initial stage of the temper-ature increment. This can probably be related to the non-stability of the solar room conditions, such as the air circulation or solar irradiation power, which may contribute to the lower surface tem-perature of the solar panel compared to simulations. At the equilib-rium conditions without water ﬂow, the FEM simulations have good agreement with the experiment data with less than 2.5% dif-ference. At the temperature falling region after the water ﬂow introduced, the temperature ﬂuctuation of the experiment data is due to the variations of the water ﬂow rate, which is difﬁcult to control at low ﬂow rate. Better ﬁttings inFig. 9(b) can be achieved at high water ﬂow rate, e.g. 66 ml/min, which normally is more stable compared to 33 ml/min.
3.4. Energy efﬁciency analysis
From the simulation and experimental data, it is found that FGM based water tubes can effectively reduce the panel tempera-ture. For the case of 1100 W/m2irradiation with 66 ml/min water ﬂow, the panel temperature can be reduced from 55 to 35 °C (aver-age from 32 to 38 °C). The single crystalline Si solar cell efﬁciency is 13 % at room temperature and normally decreases with tempera-ture. Based on the crystalline Si cell efﬁciency temperature coefﬁ-cient of 0.54 %/°C characterized in another work , the efﬁciency of the PV cell will downgrade to 10.8% at 55 °C and re-cover to 12.3% at 35 °C with the FGM cooling function. So that the PV cell performance can keep around 95% of that at room tem-perature even under 1100 W/m2 irradiation. Using the 25 point
irradiation value inFig. 3, the total input solar energy Einon the pa-nel can be numerically calculated to be 93.9 W and electric energy generated from PV cell is Epv= Ein 12.3% = 11.5 W. In addition, the thermal energy collected by water per second is around Ewater= mwater Cwater Twater= 1.1 g 4.18 W/g °C 12 °C = 55.2 W. (The outlet water temperature in around 32 °C based onFig. 6(b)). Thus the overall efﬁciency of the panel is
g= (Ewater+ Epv)/Ein= (55.2 + 11.5)/93.9 = 71%, which are very promising results com-pared to those of traditional PV thermal hybrid solar panels. The energy efﬁciency analysis and comparisons with traditional panels are summarized inTable 2.
A novel solar panel integrated with photovoltaic cells and water tubes embedded in functionally graded material (FGM) is fabri-cated. The FGM layer can effectively transfer heat from the PV cells to water tubes and prevent heat loss to the substrate. The hybrid solar panel exhibits promising performance with PV cells working at relatively low temperatures. Considering electricity and thermal energy collection, the overall panel efﬁciency is around 71%, which compares favorably with those of traditional PV thermal hybrid so-lar panels. A ﬁnite element model was successfully built to simu-late the heat transfer characteristics in the hybrid solar panel prototype and the simulation results are consistent with the exper-imental data. It provides a general approach for future FGM based solar panel design and optimization.
This work is sponsored by the National Science Foundation CMMI 0954717 and Department of Energy STTR DE-SC0003347, whose support is gratefully acknowledged. The authors are also grateful to Liming Li and Adrian Brügger, managers of Carleton Laboratory, for their strong support on the solar panel fabrication and testing. In addition, students Pablo Presto-Munoz, Michael Lackey, Alaa Saleh, and Steven Wong participated in the fabrication of hybrid solar panel prototypes, Michael Shields participated in the test design, Greg Kelly from Weidlinger Associates Inc. and Jac-ques Garant from HLW International participated in the water tube connection. The contribution from all of them is highly appreciated.
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